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In summary, the random matrices discussed in Section 1 share a common structure on the joint distributions of their eigenvalues.
Next, we verify the proposition above with random matrices discussed in Section 1. (Let and denote two mutually independent complex Gaussian matrices).
In this section, we show that the random matrices discussed in Section 1 share a common structure on the joint probability density functions (PDFs) of their eigenvalues.
Compound sets used to generate the matrices discussed in the paper are made available as a part of the revision (via ZENODO, please see ref. 16).
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Secondly, column [2] presents the Sys-GMM results using the weighting matrix discussed in Blundell and Bond (1998).
Let denote a Hermitian random matrix discussed in Section 1, and let,, denote the nonzero ordered eigenvalues of .
{partial mathbf {g}(mathbf {m}) over partial mathbf {m}} right| _{mathbf {m}=mathbf {m}_k}), is the appropriate Jacobian matrix, (underline{underline{mathbf {R}}}) is a regularisation matrix discussed in detail below, and (underline{underline{mathbf {W}}}_{k}) is a (Huber) weighting matrix.
Key factors within dECMs, consisting of microarchitecture characteristics and micromechanical properties as well as retained insoluble and soluble matrix components, are discussed in-depth for potential mechanisms underlying the functionality of these dECMs in regulating chondrogenesis.
The types of genomic relationship matrices studied here are on the form (1) as in VanRaden [ 3], but other types of genomic relationship matrices are discussed in the discussion section.
The computation of a basis of this quotient space using the bases for and can be done with integer matrix decompositions of the boundary operator matrices, as discussed in [7, 8].
Digestion methods in biological and environmental matrices were discussed in our previous studies [47, 48].
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